{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:S5YI64MZT52ACY4IFG6I4JWVDW","short_pith_number":"pith:S5YI64MZ","schema_version":"1.0","canonical_sha256":"97708f71999f7401638829bc8e26d51dbd7c4aaf333d7af00945c024a47ac2e7","source":{"kind":"arxiv","id":"1110.0877","version":2},"attestation_state":"computed","paper":{"title":"Spin Ice: Magnetic Excitations without Monopole Signatures using Muon Spin Rotation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. A. Aczel, A. Dabkowski, B. Javanparast, C. Arguello, D. J. Singh, F. L. Ning, G. M. Luke, H. Dabkowska, H. M. L. Noad, M.-H. Du, M. J. P. Gingras, S. R. Dunsiger, T. Goko, T. J. Williams, T. Lin, Y. J. Uemura","submitted_at":"2011-10-05T00:49:46Z","abstract_excerpt":"Theory predicts the low-temperature magnetic excitations in spin ices consist of deconfined magnetic charges, or monopoles. A recent transverse-field (TF) muon spin rotation (muSR) experiment [S T Bramwell et al, Nature 461, 956 (2009)] reports results claiming to be consistent with the temperature and magnetic field dependence anticipated for monopole nucleation - the so-called second Wien effect. We demonstrate via a new series of muSR experiments in Dy_2Ti_2O_7 that such an effect is not observable in a TF muSR experiment. Rather, as found in many highly frustrated magnetic materials, we ob"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1110.0877","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-10-05T00:49:46Z","cross_cats_sorted":[],"title_canon_sha256":"e747985cf9bb6f5e3b70e1c09bfd0f8daec977836f8e6448a10f8193b2ff705d","abstract_canon_sha256":"74ff3fdbe02a4996c53d71485e45af7d32c5f01e72b0c570dfda7710651803d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:08:03.403010Z","signature_b64":"uEZ+RSEY/E6+LOr8NfneKtlHRjP5ebPOkDFc9znzyf19FLZH6lqQM+wHmYD7v1QoX/yxFJYrc5P4PRNjfgDvDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"97708f71999f7401638829bc8e26d51dbd7c4aaf333d7af00945c024a47ac2e7","last_reissued_at":"2026-05-18T04:08:03.402564Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:08:03.402564Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin Ice: Magnetic Excitations without Monopole Signatures using Muon Spin Rotation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. A. Aczel, A. Dabkowski, B. Javanparast, C. Arguello, D. J. Singh, F. L. Ning, G. M. Luke, H. Dabkowska, H. M. L. Noad, M.-H. Du, M. J. P. Gingras, S. R. Dunsiger, T. Goko, T. J. Williams, T. Lin, Y. J. Uemura","submitted_at":"2011-10-05T00:49:46Z","abstract_excerpt":"Theory predicts the low-temperature magnetic excitations in spin ices consist of deconfined magnetic charges, or monopoles. A recent transverse-field (TF) muon spin rotation (muSR) experiment [S T Bramwell et al, Nature 461, 956 (2009)] reports results claiming to be consistent with the temperature and magnetic field dependence anticipated for monopole nucleation - the so-called second Wien effect. We demonstrate via a new series of muSR experiments in Dy_2Ti_2O_7 that such an effect is not observable in a TF muSR experiment. Rather, as found in many highly frustrated magnetic materials, we ob"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.0877","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1110.0877","created_at":"2026-05-18T04:08:03.402622+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.0877v2","created_at":"2026-05-18T04:08:03.402622+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.0877","created_at":"2026-05-18T04:08:03.402622+00:00"},{"alias_kind":"pith_short_12","alias_value":"S5YI64MZT52A","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"S5YI64MZT52ACY4I","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"S5YI64MZ","created_at":"2026-05-18T12:26:41.206345+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW","json":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW.json","graph_json":"https://pith.science/api/pith-number/S5YI64MZT52ACY4IFG6I4JWVDW/graph.json","events_json":"https://pith.science/api/pith-number/S5YI64MZT52ACY4IFG6I4JWVDW/events.json","paper":"https://pith.science/paper/S5YI64MZ"},"agent_actions":{"view_html":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW","download_json":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW.json","view_paper":"https://pith.science/paper/S5YI64MZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.0877&json=true","fetch_graph":"https://pith.science/api/pith-number/S5YI64MZT52ACY4IFG6I4JWVDW/graph.json","fetch_events":"https://pith.science/api/pith-number/S5YI64MZT52ACY4IFG6I4JWVDW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW/action/storage_attestation","attest_author":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW/action/author_attestation","sign_citation":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW/action/citation_signature","submit_replication":"https://pith.science/pith/S5YI64MZT52ACY4IFG6I4JWVDW/action/replication_record"}},"created_at":"2026-05-18T04:08:03.402622+00:00","updated_at":"2026-05-18T04:08:03.402622+00:00"}